E. Obryadina, N. Sidorov, N. Teplyakova, M. Palatnikov
{"title":"铁电Li0.12Na0.88TayNb1−yO3固溶体的结构相变和“有序-无序”过程","authors":"E. Obryadina, N. Sidorov, N. Teplyakova, M. Palatnikov","doi":"10.1109/OMEE.2012.6464821","DOIUrl":null,"url":null,"abstract":"The system of the Li<inf>x</inf>Na<inf>1−x</inf>Ta<inf>y</inf>Nb<inf>1−y</inf>O<inf>3</inf> solid solutions based on sodium niobate with oxygen-octahedral type of structure is of great interest because the changes of the components concentration and the temperature are accompanied by a variety of structural phase transitions. Particularly, the Li<inf>0.12</inf>Na<inf>0.88</inf>Ta<inf>y</inf>Nb<inf>1−y</inf>O<inf>3</inf> solid solution is promising as a material with high superionic conductivity. When x = 0.12 the structure orders in such a way as to make the phase transition to the superionic state possible. Besides, at temperatures 315–350 °C in the Li<inf>0.12</inf>Na<inf>0.88</inf>Ta<inf>y</inf>Nb<inf>1−y</inf>O<inf>3</inf> solid solution the phase transition from ferroelectric to antiferroelectric phase taking place before the superionic one can be observed. They were found at ∼ 400÷460 °C.","PeriodicalId":6332,"journal":{"name":"2012 IEEE International Conference on Oxide Materials for Electronic Engineering (OMEE)","volume":"35 1","pages":"122-123"},"PeriodicalIF":0.0000,"publicationDate":"2012-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Structural phase transitions and processes of “order-disorder” in the ferroelectric Li0.12Na0.88TayNb1−yO3 solid solution\",\"authors\":\"E. Obryadina, N. Sidorov, N. Teplyakova, M. Palatnikov\",\"doi\":\"10.1109/OMEE.2012.6464821\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The system of the Li<inf>x</inf>Na<inf>1−x</inf>Ta<inf>y</inf>Nb<inf>1−y</inf>O<inf>3</inf> solid solutions based on sodium niobate with oxygen-octahedral type of structure is of great interest because the changes of the components concentration and the temperature are accompanied by a variety of structural phase transitions. Particularly, the Li<inf>0.12</inf>Na<inf>0.88</inf>Ta<inf>y</inf>Nb<inf>1−y</inf>O<inf>3</inf> solid solution is promising as a material with high superionic conductivity. When x = 0.12 the structure orders in such a way as to make the phase transition to the superionic state possible. Besides, at temperatures 315–350 °C in the Li<inf>0.12</inf>Na<inf>0.88</inf>Ta<inf>y</inf>Nb<inf>1−y</inf>O<inf>3</inf> solid solution the phase transition from ferroelectric to antiferroelectric phase taking place before the superionic one can be observed. They were found at ∼ 400÷460 °C.\",\"PeriodicalId\":6332,\"journal\":{\"name\":\"2012 IEEE International Conference on Oxide Materials for Electronic Engineering (OMEE)\",\"volume\":\"35 1\",\"pages\":\"122-123\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2012-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2012 IEEE International Conference on Oxide Materials for Electronic Engineering (OMEE)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/OMEE.2012.6464821\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2012 IEEE International Conference on Oxide Materials for Electronic Engineering (OMEE)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/OMEE.2012.6464821","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Structural phase transitions and processes of “order-disorder” in the ferroelectric Li0.12Na0.88TayNb1−yO3 solid solution
The system of the LixNa1−xTayNb1−yO3 solid solutions based on sodium niobate with oxygen-octahedral type of structure is of great interest because the changes of the components concentration and the temperature are accompanied by a variety of structural phase transitions. Particularly, the Li0.12Na0.88TayNb1−yO3 solid solution is promising as a material with high superionic conductivity. When x = 0.12 the structure orders in such a way as to make the phase transition to the superionic state possible. Besides, at temperatures 315–350 °C in the Li0.12Na0.88TayNb1−yO3 solid solution the phase transition from ferroelectric to antiferroelectric phase taking place before the superionic one can be observed. They were found at ∼ 400÷460 °C.